...L t q q k j , , 2 , 1 L 称为拉格朗日函数(Lagrangian function)或动势 (Kinetic potential) 主动力为有势力的拉格朗日方程 拉格朗日方程是以广义坐标表示的动力学普遍方 程,适用于理想完整约束的任意质点系。
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potential of Kinetic State 称为动态位
Kinetic Energy and Potential Energy 动能与位能
kinetic and potential energy 动能与势能 ; 意为“动能与势能”
kinetic shielding potential 动屏蔽势
So what, now, is then the total -- energy of the system-- that is, the sum of the kinetic energy plus the potential energy?
所以现在系统内,总能量是多少-,是动能和,势能之和吗?
That means the sum of potential energy and kinetic energy.
总功指的是势能,和动能的总和。
Then we have the conservation - of mechanical energy — the sum of kinetic energy and potential energy.
我们知道,机械能守恒定律-,动能和,势能的总和。
The total energy of the system, which we are going to get from postulate number four, which says the energy of the electron, which is the energy of the system, is the sum of the kinetic and the potential energy.
这个系统的总能量,也就是我们将从第四个假设中算出的能量,也就是电子运动产生的能量,也就是整个系统的能量,是动能和位能的总和。
It means that we better get away from these deterministic models where we have a little electron here with its potential energy and its kinetic energy.
它的意思是我们最好远离,这些确定性模型,那里有一个小电子,它具有势能和动能。
And we know that n describes the total energy, that total binding energy of the electron, so the total energy is going to be equal to potential energy plus kinetic energy.
我们知道,n是描述总能量的,电子总的结合能,所以总能量,等于,势能加动能。
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